TECHNICAL FIELD
The present disclosure relates to image sensors. The present disclosure is particularly applicable to backside illumination (BSI) visible light sensors and single-photon avalanche diode (SPAD) detectors.
BACKGROUND
When BSI visible light sensors and SPAD detectors are fabricated on the same substrate, their detector density is reduced because the substrate area is shared between two different types of detectors. Further, resolution and pixel density for both BSI visible light sensors and SPAD detectors are reduced.
A need therefore exists for an image sensor with improved resolution and pixel density, and for enabling methodology.
SUMMARY
An aspect of the present disclosure is a device including a SPAD detector and a BSI visible light sensor positioned on different planes, the device exhibiting improved resolution and pixel density.
Another aspect of the present disclosure is a method of forming a device including a SPAD detector and a BSI visible light sensor positioned on different planes, the device exhibiting improved resolution and pixel density.
Additional aspects and other features of the present disclosure will be set forth in the description which follows and in part will be apparent to those having ordinary skill in the art upon examination of the following or may be learned from the practice of the present disclosure. The advantages of the present disclosure may be realized and obtained as particularly pointed out in the appended claims.
According to the present disclosure, some technical effects may be achieved in part by a device including: a photodiode for detecting visible light; and a SPAD detector for detecting infrared (IR) radiation, wherein the photodiode and the SPAD detector are on different planes.
Another aspect of the present disclosure is a method including: forming a BSI visible light sensor with a crystalline vertical transfer gate (VTG) channel in a first tier; forming a SPAD detector in a second tier; and bonding the first tier and the second tier, wherein the crystalline VTG channel transfers a charge from the BSI visible light sensor to a read out circuitry in the second tier.
A further aspect of the present disclosure is device including: a BSI visible light sensor with a crystalline VTG channel in a first tier for detecting visible light; a SPAD detector in a second tier for detecting IR radiation; and the first tier bonded to the second tier, wherein the BSI visible light sensor and the SPAD detector are positioned such that a charge generated in the BSI visible light sensor is transferred by the crystalline VTG channel to a read out circuitry in the second tier.
Additional aspects and technical effects of the present disclosure will become readily apparent to those skilled in the art from the following detailed description wherein embodiments of the present disclosure are described simply by way of illustration of the best mode contemplated to carry out the present disclosure. As will be realized, the present disclosure is capable of other and different embodiments, and its several details are capable of modifications in various obvious respects, all without departing from the present disclosure. Accordingly, the drawings and description are to be regarded as illustrative in nature, and not as restrictive.
BRIEF DESCRIPTION OF THE DRAWINGS
The present disclosure is illustrated by way of example, and not by way of limitation, in the figures of the accompanying drawing and in which like reference numerals refer to similar elements and in which:
FIGS. 1 through 7 illustrate cross-sectional views of a process flow for forming a BSI visible light sensor with a crystalline VTG channel, in accordance with an exemplary embodiment;
FIG. 8 illustrates a cross-sectional view of a SPAD detector and a portion of read out circuitry for BSI visible light sensors, in accordance with an exemplary embodiment; and
FIGS. 9 and 10 illustrate cross-sectional views of a process flow for bonding the BSI visible light sensor to the SPAD detector, in accordance with an exemplary embodiment.
DETAILED DESCRIPTION
In the following description, for the purposes of explanation, numerous specific details are set forth in order to provide a thorough understanding of exemplary embodiments. It should be apparent, however, that exemplary embodiments may be practiced without these specific details or with an equivalent arrangement. In other instances, well-known structures and devices are shown in block diagram form in order to avoid unnecessarily obscuring exemplary embodiments. In addition, unless otherwise indicated, all numbers expressing quantities, ratios, and numerical properties of ingredients, reaction conditions, and so forth used in the specification and claims are to be understood as being modified in all instances by the term “about.”
The present disclosure addresses and solves the current problem of reduced resolution and pixel density attendant upon forming the BSI visible light sensors and SPAD detectors on the same substrate. The problem is solved, inter alia, by forming SPAD detector and BSI visible light sensor on different substrate/planes.
Methodology in accordance with embodiments of the present disclosure includes a photodiode for detecting visible light, and a SPAD detector for detecting IR radiation. The photodiode and the SPAD detector are formed on different planes.
Still other aspects, features, and technical effects will be readily apparent to those skilled in this art from the following detailed description, wherein preferred embodiments are shown and described, simply by way of illustration of the best mode contemplated. The disclosure is capable of other and different embodiments, and its several details are capable of modifications in various obvious respects. Accordingly, the drawings and description are to be regarded as illustrative in nature, and not as restrictive.
FIGS. 1 through 7 illustrate cross-sectional views of a process flow for forming a BSI visible light sensor with a crystalline VTG channel, in accordance with an exemplary embodiment. Referring to FIG. 1, STI regions 101 are formed in a first tier substrate 103 (herein after substrate 103), e.g., formed of silicon (Si), germanium (Ge), indium gallium arsenide (InGaAs) or any other material with similar functional properties. The STI regions 101 are filled with insulating material, e.g., silicon dioxide (SiO2), silicon nitride (SiN) or any other material with similar functional properties, electrically isolating regions in the substrate 103. Then, an N+ layer 105 is formed, e.g., by N-type dopants phosphorus (P), arsenic (As) or any other material with similar functional properties, within the substrate 103. Thereafter, a portion of the substrate 103 and the N+ layer 105 are etched, forming a fin 107. In one instance, the lower portion of the fin 107 includes N+ layer 105 and the upper portion of the fin 107 includes substrate 103. Subsequently, a P+ layer 109 is formed, e.g., by P-type dopants boron (B), indium (In) or any other material with similar functional properties, in an upper surface of the N+ layer 105 and the fin 107.
Thereafter, an oxide layer is formed over the P+ layer 109 and the fin 107 between the STI regions 101. Then, the oxide layer and the P+ layer 109 in an upper surface of the fin 107 are planarized, e.g., by chemical mechanical planarization (CMP) or like processes, forming fin 107′, as represented in FIG. 2. In this instance, the upper surface of the oxide layer is substantially coplanar to the upper surface of the fin 107′ (not shown for illustrative convenience). Next, a portion of the oxide layer and the STI regions 101 are etched below the lower portion of the fin 107′, forming STI regions 101′ and oxide layer 201. As depicted in FIG. 3, a gate dielectric layer 301 is formed, e.g., of silicon oxide, silicon nitride (Si3N4), hafnium oxide (HfO2) or any other material with similar functional properties, over and along the fin 107′ and portions of the oxide layer 201. In one instance, the surface of the fin 107′ is treated for roughness prior to forming the gate dielectric layer 301.
Referring to FIG. 4, a gate layer is formed, e.g., of polycrystalline silicon, titanium (Ti), tantalum nitride (TaN), indium oxide (In2O3) or any other material with similar functional properties, over the STI regions 101′, the oxide layer 201 and the gate dielectric layer 301. Next, the gate layer is etched, e.g., by dry etching or a combination of CMP and dry etching, below an upper surface of the fin 107′, forming the gate layer 401. Thereafter, the gate layer 401 is patterned (not shown for illustrative convenience). In one instance, the gate layer 401 may include a non-transparent gate material that is etched and patterned to minimize the coverage on top of the P+ layer 109, i.e., a visible light sensor. Then, a dielectric layer 501 is formed, e.g., of nitride, oxide or any other material with similar functional properties, over the gate layer 401 and gate dielectric layer 301, as depicted in FIG. 5. Then, the dielectric layer 501 and the gate dielectric layer 301 are planarized, e.g., by CMP or like processes, down to the upper surface of the fin 107′, forming gate dielectric layer 301′ and gate dielectric layer 501′, as illustrated in FIG. 6. Subsequently, a Si floating node (FN) layer 601 is formed, e.g., by epitaxy or polysilicon deposition, over the fin 107′, the gate dielectric layer 301′ and portions of the dielectric layer 501′. Subsequently, the Si FN layer 601 is doped with N-type dopants. In one instance, the Si FN layer 601 and the fin 107′ forms a T-shaped crystalline VTG channel 603.
Next, in FIG. 7, an oxide layer 701 is formed over the gate dielectric layer 501′ and the Si FN layer 601. Thereafter, contact 703 is formed through the oxide layer 701 and the dielectric layer 501′ to the gate layer 401; and contact 705 is formed through the oxide layer 701 to the Si FN layer 601. In one instance, the contacts 703 and 705 are filled with tungsten (W), copper (Cu) or any other material with similar functional properties. Then, an oxide layer 707 is conformally deposited over the oxide layer 701. Thereafter, a metal layer 709 is formed in the oxide layer 707 and above the contacts 703 and 705. Next, an oxide layer 711 is formed over the oxide layer 707 and the metal layer 709. Subsequently, vias 713 and 715 are formed through the oxide layer 711 to the metal layer 709. This process can be repeated to form the necessary back end of line (BEOL) process as required. Accordingly, a BSI visible light sensor 717 is formed in a first tier.
FIG. 8 illustrates a cross-sectional view of a SPAD detector and a portion of read out signal structure for the BSI visible light sensors, in accordance with an exemplary embodiment. Referring to FIG. 8, an N+ region 801, and 803 are formed, e.g., by N-type dopants P, As or any other material with similar functional properties, in a second tier substrate 805 (herein after substrate 805), e.g., formed of Si, Ge, InGaAs or any other material with similar functional properties. Next, a P+ layer 807 is formed, e.g., by P-type dopants B or In, in an upper surface of the N+ region 803. Thereafter, an oxide layer 809 is formed over the substrate 805, the N+ region 801, the P+ layer 807 and the N+ region 803. Subsequently, contacts 811, 813 and 815 are formed, e.g., with similar process as contacts 703 and 705, through the oxide layer 809 down to the N+ region 801, the P+ layer 807 and the N+ region 803, respectively. Similarly, a substrate contact is formed (not shown for illustrative convenience). Consequently, a metal layer 817 is formed, e.g., of Cu, Al or any other material with similar functional properties, in the oxide layer 809. In one instance, multiple levels of oxide, vias and metal layers can be repeatedly formed depending on BEOL requirement. Accordingly, a SPAD detector 819 is formed in a second tier. In one instance, the SPAD detector 819 is surrounded by other SPAD detectors (not shown for illustrative convenience). In another instance, the SPAD detector 819 includes an application specific integrated circuit (ASIC) layer for a two-dimensional (2D) or three-dimensional (3D) data readout. In a further instance, the ASIC layer may be fabricated on a separate third tier substrate to which the substrate 103 and 805 may be bonded.
FIGS. 9 and 10 illustrate cross-sectional views of a process flow for bonding the BSI visible light sensor to the SPAD detector, in accordance with an exemplary embodiment. The BSI visible light sensor 717 is flipped as shown in FIG. 9, thereafter, in FIG. 10, the FN contact 705 and the gate contact 703 of the BSI visible light sensor 717 is aligned with contact 811 and metal layer 817 in the same tier as the SPAD detector 819, respectively. The subsequent metal connection to contacts 813 and 815 is not shown for illustrative convenience. The oxide layer 711 of the BSI visible light sensor 717 is bonded, e.g., by through silicon via (TSV), Cu—Cu bonding or like processes, with the oxide layer 809 of the SPAD detector 819. Then, bottom portion of substrate 103 is planarized and thinned, e.g., by backside CMP or like processes, and is followed by a backside treatment. Subsequently, a filter 1001, e.g., color filters, is attached over the bottom surface of the substrate 103 to improve the sensitivity of the BSI visible light sensor 717. In addition, micro-lense 1003 may be attached to the filter 1001 per requirement. In one instance, the crystalline VTG channel 603 transfers a charge from the BSI visible light sensor 717 to the read out circuit (not shown for illustrative convenience) via the N+ region 801, fabricated in the second tier. In another instance, the IR sensing by SPAD detector 819 is used for depth sensing to produce a 3D image. In a further instance, a light first passes through the BSI visible light sensor 717 and then the SPAD detector 819. The SPAD detector 819 allows passage of a specified wavelength or a wavelength more than 850 nanometer (nm).
The embodiments of the present disclosure can achieve several technical effects, such as improved resolution and pixel density because BSI visible light sensors and SPAD detectors are formed on separate tiers or planes. Further, the present disclosure achieves higher fill factor and mobility because the VTG includes a crystalline channel. In addition, performance for each detector can be optimized separately based on the target wavelength or absorption depth. For example, the SPAD detector can utilize a much deeper silicon depth which is beneficial for IR detection. Devices formed in accordance with embodiments of the present disclosure enjoy utility in various industrial applications, e.g., microprocessors, smart phones, mobile phones, cellular handsets, set-top boxes, DVD recorders and players, automotive navigation, printers and peripherals, networking and telecom equipment, gaming systems, and digital cameras. The present disclosure enjoys industrial applicability in any of various types of integrated semiconductor devices or image sensors.
In the preceding description, the present disclosure is described with reference to specifically exemplary embodiments thereof. It will, however, be evident that various modifications and changes may be made thereto without departing from the broader spirit and scope of the present disclosure, as set forth in the claims. The specification and drawings are, accordingly, to be regarded as illustrative and not as restrictive. It is understood that the present disclosure is capable of using various other combinations and embodiments and is capable of any changes or modifications within the scope of the inventive concept as expressed herein.